• Title/Summary/Keyword: 반사경계

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A Study on the Vibration Reduction Effect of a Soil Grouting (지반내 그라우팅공법에 의한 지반진동감소 연구)

  • Huh, Young;Cho, Jun-Sang;Koo, Yong-Woo
    • Proceedings of the Korean Society for Noise and Vibration Engineering Conference
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    • 1995.10a
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    • pp.104-110
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    • 1995
  • 지반과 구조물의 동적 상호작용은 건설분야에서의 중요한 현상으로, 특히 지반을 통해 인근구조물로 전달되는 진동은 구조물 자체의 구조적인 문제 뿐 아니라 그 속에 거주하는 사람이나 설비에 대한 안전성 또는 사용성에 나쁜 영향을 야기할 수 있다. 본 논문에서는 이러한 진동을 저감시키기 위해, 지반내에 정상적인 진동전파를 방해하는 구조물을 시공하여 진동 저감효과를 만들어 내는 방법을 연구하였다. 이러한 연구의 발상은 다음과 같다. 충진지반에서의 지반진동의 진폭을 해석하면서 진동의 크기가 기저암의 위치에 따라 큰 영향을 받는 것을 알았고 이로부터 지반내에 인위적인 층을 만들수 있다면 지반진동의 크기를 변화시킬 수 있지 않을까라는 생각에서 본 연구를 시작하였다. 또한 지반 내에서의 정상적인 진동의 전파를 방해하기 위한 차진 구조물을 만드는 방법은 연약지반의 강도중대 또는 차수의 목적으로 주로 사용하고 있는 그라우팅공법의 사용이 가능할 것이므로, 기존의 그라우팅현장에서 만들어진 지반의 물성치들을 사용하여 경계요소법에 의한 수치해석적 방법을 택하였다. 본 연구에서는 그라우팅공법의 시공성에 관한 것은 포함되지 않는다. 본 논문에서는 지반의 구조를 경사구조와 수평지반구조라는 두가지 특징적인 경우에 대해 검토하였다. 이중 경사진 기저암층을 가진 지반의 경우에는 기저암에서 진동의 비대칭적인 반사에 의해 수평기저암에서와는 달리 기저암의 한쪽에서 다른쪽에 비해 큰 진동이 발생한다. 그라우팅층의 효과를 검토하기 위한 연구의 순서는 일정주파수의 조화진동에 대해 먼저 여러 가지 크기의 그라우팅층과 함께 블록으로 볼 수 있는 크기의 그라우팅층에 대해 진동저감효과를 해석하였고, 이를 통해 보강층의 소요크기 및 최적위치를 구하였다. 사용된 물성치는 실제 지하철 건설현장에서 나타난 지반물성치 및 그라우팅후의 지반강도 및 전단파전파속도를 이용하였다. 또한 마지막에서 검토된 기차하중에 대한 효과를 알아보기 위해 사용된 기차운행에 의한 지반가속도도 역시 측정된 값을 사용하였다. 그러나 당시의 기차운행속도가 낮아 정상적인 운행에서는 더 큰 값이 나올 것으로 판단되었으나 측정된 값을 그대로 사용하였다.

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Prestack Reverse Time Migration for Seismic Reflection data in Block 5, Jeju Basin (제주분지 제 5광구 탄성파자료의 중합전 역시간 구조보정)

  • Ko, Chin-Surk;Jang, Seong-Hyung
    • Economic and Environmental Geology
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    • v.43 no.4
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    • pp.349-358
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    • 2010
  • For imaging complex subsurface structures such as salt dome, faults, thrust belt, and folds, seismic prestack reverse-time migration in depth domain is widely used, which is performed by the cross-correlation of shot-domain wavefield extrapolation with receiver-domain wavefield extrapolation. We apply the prestack reverse-time migration, which had been developed at KIGAM, to the seismic field data set of Block 5 in Jeju basin of Korea continental shelf in order to improve subsurface syncline stratigraphy image of the deep structures under the shot point 8km at the surface. We performed basic data processing for improving S/N ratio in the shot gathers, and constructed a velocity model from stack velocity which was calculated by the iterative velocity spectrum. The syncline structure of the stack image appears as disconnected interfaces due to the diffractions, but the result of the prestack migration shows that the syncline image is improved as seismic energy is concentrated on the geological interfaces.

Temperature Effect on the Physical Properties of Boryung Sandstone and Yeosan Marble (보령사암과 여산대리암의 물리적 특성에 대한 온도의 영향)

  • Yoon Yong-Kyun
    • Explosives and Blasting
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    • v.22 no.4
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    • pp.17-22
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    • 2004
  • Boryung sandstone and Yeosan marble were thermally cracked at predetermined temperatures ranging $200^{\circ}C$ to $600^{\circ}C$. Optical microscopy was utilized to observe thermally induced cracks and physical properties such as specific gravity, effective porosity k elastic wave velocity were measured. Optical observations show that all crystal boundaries of Yeosan marble heated to $600^{\circ}C$ open and new intracrystalline cracks seem to be occurred in all crystals, but developments of thermal cracks in Boryung sandstone heated to $600^{\circ}C$ are not pronounced. From $200^{\circ}C$ upwards, effective porosity and elastic wave velocity of Yeosan marble are sharpely increased, whereas effective porosity and elastic wave velocity of Boryung sandstone are weakly increased.

Numerical Simulation of Dynamic Soil-pile-structure Interaction in Liquefiable Sand (액상화 가능한 지반에 근입된 지반-말뚝-구조물 동적 상호작용의 수치 모델링)

  • Kwon, Sun-Yong;Yoo, Min-Taek;Kim, Seok-Jung
    • Journal of the Korean Geotechnical Society
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    • v.34 no.7
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    • pp.29-38
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    • 2018
  • Three-dimensional continuum modeling of dynamic soil-pile-structure interaction embedded in a liquefiable sand was carried out. Finn model which can model liquefaction behavior using effective stress method was adopted to simulate development of pore water pressure according to shear deformation of soil directly in real time. Finn model was incorporated into Non-linear elastic, Mohr-Coulomb plastic model. Calibration of proposed modeling method was performed by comparing the results with those of the centrifuge tests performed by Wilson (1998). Excess pore pressure ratio, pile bending moment, pile head displacement-time history according to depth calculated by numerical analysis agreed reasonably well with the test results. Validation of the proposed modeling method was later performed using another test case, and good agreement between the computed and measured values was observed.

Design of a 3:1 Wideband Circular Polarizer with Multilayered Meanderline Using Hybrid Method (하이브리드 방법을 이용한 다층 미앤더선로 구조의 3:1 광대역 원편파 편파기 설계)

  • Lee, Cheol-Soo;Pack, Jeong-Ki
    • The Journal of Korean Institute of Electromagnetic Engineering and Science
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    • v.26 no.8
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    • pp.730-739
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    • 2015
  • In this paper, a wideband circular polarizer operating in the frequency range of 6~18 GHz is designed and fabricated using a multilayer structure with meanderlines. A T matrix expression for the unit structure, which consists of meanderline, dielectric substrate and spacer, was derived using the boundary value solution. A proposed meanderline structure was modeled as an array of unit meanderline cell in order to apply the waveguide model with PEC and PMC boundary conditions. The calculation procedures to obtain an equivalent susceptance of the unit meanderline cell using HFSS was also suggested. Using a hybrid method, which combines the T matrix with the HFSS results, and cut-and-try method, a wideband circular polarizer with low insertion loss and good AR performance was designed. The fabricated polarizer has the return loss less than -10 dB within 92 % bandwidth, the average insertion loss less than -0.24 dB, and the average AR below 2.6 dB for full 3:1 bandwidth.

Numerical Simulation of the Effect of Finite Diaphragm Rupture Process on Micro Shock Tube Flows (Micro shock tube 유동에 대한 유한 격막 파막과정의 영향에 관한 수치 해석적 연구)

  • Arun Kumar, R.;Kim, Heuy Dong
    • Journal of the Korean Society of Propulsion Engineers
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    • v.17 no.3
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    • pp.37-46
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    • 2013
  • Recent years have witnessed the use of micro shock tube in various engineering applications like micro combustion, micro propulsion, particle delivery systems etc. The flow characteristics occurring in the micro shock tube shows a considerable deviation from that of well established conventional macro shock tube due to very low Reynolds number and high Knudsen number effects. Also the diaphragm rupture process, which is considered to be instantaneous process in many of the conventional shock tubes, will be crucial for micro shock tubes in determining the near diaphragm flow field and shock formation. In the present study, an axi-symmetric CFD method has been applied to simulate the micro shock tube, with Maxwell's slip velocity and temperature jump boundary conditions. The effects of finite diaphragm rupture process on the flow field and the shock formation was investigated, in detail. The results show that the shock strength attenuates rapidly as it propagates through micro shock tubes.

A case study of 3D seismic reflection imaging in an area of ground subsidence (지반 침하지역에서의 3차원 탄성파 반사법에 의한 지하구조 영상화 사례)

  • Ko, Kwang-Beom;Lee, Doo-Sung
    • 한국지구물리탐사학회:학술대회논문집
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    • 2000.09a
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    • pp.158-172
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    • 2000
  • In order to visualize mine cavities, 3D seismic reflection data were acquired at the ground subsidence sites near Nampung coal mine area, Neukguri, Dogye, Samchuck. Full range 3D array with complete range of azimuths on the bins was considered in the data acquisition design. Because of poor S/N data, we estimated the stacking velocities by CVS method, and we estimated the shot and receiver statics on the shot and receiver stack data. We could confirm that features of ground collapse that were expected from the subsidence. In order to visualize the cavities, we need to apply more sophisticated processing schemes, such as velocity analysis, residual statics correction.

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Super-RENS Readout Signal Simulation (Super-RENS 재생 신호 계산)

  • Lee, Jin-Kyung;Hwang, In-Oh;Kim, Hyun-Ki;Bae, Jae-Cheol;Kim, Joo-Ho
    • Transactions of the Society of Information Storage Systems
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    • v.3 no.1
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    • pp.34-39
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    • 2007
  • Super-REsolution Near-field Structure (Super-RENS) 재생 현상을 모델링하고 재생 신호를 계산하여 실험 결과와 비교하였다. 약 2mW 내외의 높은 광 파워로 집광된 Spot 은 디스크 내의 상변화 물질인 GST 를 용융시키므로 집광 Spot 내에는 용융 영역과 비 용융 영역이 공존하게 되고 연속적 또는 불연속적인 경계를 이루게 된다. 이러한 열 효과로부터 기인하는 집광 Spot 내에서의 물질의 광학적 특성 변화와 변화 정도의 차이를 가정하였고 변화된 광학적 특성은 집광된 Spot 의 유효 크기를 줄어들게 함으로써 회절한계 이하의 정보를 재생 가능하게 한다. 계산은 FDTD 방법과 Scalar 방법을 병행하였다. FDTD 방법으로는 위와 같은 집광 Spot 내의 물질 굴절률 (n,k) 변화로부터 회절한계 이하의 정보가 재생 가능함과 CNR 문턱 현상을 확인하였고, Scalar 방법으로는 물질 굴절률을 직접 다루지 않고 굴절률 변화로부터 기인하는 광의 Amplitude 와 Phase 변화로부터 회절한계 이하의 정보가 재생 가능함을 확인하였다. 이 때 광의 Amplitude 와 Phase 변화를 모델링하기 위하여 지름, 위치, 반사율 변화량, 위상 변화량의 네가지 변수로 정의되는 광 마스크를 도입하였다. Scalar 방법을 이용하여 재생 RF 신호 등 다양한 Super-RENS 디스크의 신호를 계산 활용 할 수 있고 다음의 두가지 광학계에 대하여 계산과 실험으로 얻은 채널 특성 및 RF 신호를 비교하여 각각 오차평균 4.2%, 4.7%로 일치함을 확인하였다. 파장 659nm, NA=0.6, Min Pit Length=173nm ROM 디스크 System, 파장 405nm, NA=0.85 Min Mark Length=75nm WORM 디스크 System.

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An Empirical Study on the Land Cover Classification Method using IKONOS Image (IKONOS 영상의 토지피복분류 방법에 관한 실증 연구)

  • Sakong, Hosang;Im, Jungho
    • Journal of the Korean Association of Geographic Information Studies
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    • v.6 no.3
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    • pp.107-116
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    • 2003
  • This study investigated how appropriate the classification methods based on conventional spectral characteristics are for high resolution imagery. A supervised classification mixing parametric and non-parametric rules, a method in which fuzzy theory is applied to such classification, and an unsupervised method were performed and compared to each other for accuracy. In addition, comparing the result screen-digitized through interpretation to the classification result using spectral characteristics, this study analyzed the conformity of both methods. Although the supervised classification to which fuzzy theory was applied showed the best performance, the application of conventional classification techniques to high resolution imagery had some limitations due to there being too much information unnecessary to classification, shadows, and a lack of spectral information. Consequently, more advanced techniques including integration with other advanced remote sensing technologies, such as lidar, and application of filtering or template techniques, are required to classify land cover/use or to extract useful information from high resolution imagery.

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A Thermal Model for Silicon-on-Insulator Multilayer Structure in Silicon Recrystallization Using Tungsten Lamp (텅스텐 램프를 이용한 실리콘 재결정시의 SOI 다층구조에 대한 열적모델)

  • 경종민
    • Journal of the Korean Institute of Telematics and Electronics
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    • v.21 no.5
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    • pp.90-99
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    • 1984
  • A onetimensional distribution of the temperature and the heat source in the SOI (silicon-on-insulator) multi-layer structure illuminated by tungsten lamps from both sides was obtained by solving the heat equation in steady state on a finite difference grid using successive over-relaxation method. The heat source distribution was obtained by considering such features as spectral components of the light source, multiple reflection at the internal interfaces, temperature and frequency dependence of the light absorption coefficient, etc. The front and back surface temperatures, which are boundary conditions for the heat equation, were derived from a requirement that they satisfy the radiation conditions. The radiation flux as well as the conduction flux was considered in modelling the thermal behaviour at the internal interfaces. Since the temperature and the heat source profiles are strongly dependent upon each other, the calculation of each profile was iterated using the updated profile of the other until they are consistent with each other. The experimental temperature at the front surface of the wafer as measured by Pyrometer was about 1200$^{\circ}$K, while the simulated temperature was 1120$^{\circ}$K.

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